To find the sum of all possible values of \(\lambda\) for which the shortest distance between the given lines is \(\frac{6}{\sqrt{5}}\), we proceed as follows:
The given lines are:
The general form of the equations of the lines are:
The shortest distance \(d\)\) between two skew lines \(\mathbf{r}_1 = \mathbf{a}_1 + t\mathbf{b}_1\) and \(\mathbf{r}_2 = \mathbf{a}_2 + s\mathbf{b}_2\) is given by:
Here, \(\mathbf{a}_1 = \langle 4, -1, 0 \rangle\), \(\mathbf{b}_1 = \langle 1, 2, -3 \rangle\), \(\mathbf{a}_2 = \langle \lambda, -1, 2 \rangle\), and \(\mathbf{b}_2 = \langle 2, 4, -5 \rangle\).
First compute the cross product \((\mathbf{b}_1 \times \mathbf{b}_2)\):
\(\begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ 1 & 2 & -3 \\ 2 & 4 & -5 \end{vmatrix} = \mathbf{i}(2 \times -5 - (-3)\times 4) - \mathbf{j}(1\times -5 -(-3)\times 2) + \mathbf{k}(1\times 4 - 2\times 2)\)
\(= \mathbf{i}(-10 + 12) - \mathbf{j}(-5 + 6) + \mathbf{k}(4 - 4)\)
\(= \mathbf{i}(2) - \mathbf{j}(1) + \mathbf{k}(0)\)
\(= \langle 2, -1, 0 \rangle\)
Now, compute \((\mathbf{a}_2 - \mathbf{a}_1)\):
\(= \langle \lambda - 4, 0, 2 \rangle\)
Compute the dot product \((\mathbf{a}_2 - \mathbf{a}_1) \cdot (\mathbf{b}_1 \times \mathbf{b}_2)\):
\(= (\langle \lambda - 4, 0, 2 \rangle) \cdot \langle 2, -1, 0 \rangle\)
\(= 2(\lambda - 4) + 0\right)\)
\(= 2\lambda - 8\)
The magnitude of \((\mathbf{b}_1 \times \mathbf{b}_2)\): \(|\langle 2, -1, 0 \rangle| = \sqrt{2^2 + (-1)^2 + 0^2} = \sqrt{5}\)
Setting up the equation for the shortest distance:
\(\frac{|2\lambda - 8|}{\sqrt{5}} = \frac{6}{\sqrt{5}}\)
Therefore, \(|2\lambda - 8| = 6\)
This gives two equations:
The possible values of \(\lambda\) are \(7\) and \(1\). Therefore, the sum of all possible values is:
Sum = \(7 + 1 = 8\)
Thus, the sum of all possible values of \(\lambda\) is \(8\).
Given:
\(\int_0^1 \frac{1}{\sqrt{3 + x} + \sqrt{1 + x}} \, dx = a + b \sqrt{2} + c \sqrt{3}\)
where \(a, b, c\) are rational numbers.
Step 1. Simplifying the Integral: Consider
\(\int_0^1 \frac{1}{\sqrt{3 + x} + \sqrt{1 + x}} \, dx\)
Rationalizing the denominator:
\(\int_0^1 \frac{\sqrt{3 + x} - \sqrt{1 + x}}{(3 + x) - (1 + x)} \, dx = \int_0^1 \frac{\sqrt{3 + x} - \sqrt{1 + x}}{2} \, dx\)
Therefore:
\(= \frac{1}{2} \int_0^1 \left( \sqrt{3 + x} - \sqrt{1 + x} \right) \, dx\)
Step 2. Separating the Integral:
\(= \frac{1}{2} \left( \int_0^1 \sqrt{3 + x} \, dx - \int_0^1 \sqrt{1 + x} \, dx \right)\)
Step 3. Evaluating Each Integral:
- For \(\int_0^1 \sqrt{3 + x} \, dx \:\)
\(\int \sqrt{3 + x} \, dx = \frac{2}{3} (3 + x)^{3/2}\)
Evaluating from 0 to 1:
\(\frac{2}{3} \left( (3 + x)^{3/2} \right) \Big|_0^1 = \frac{2}{3} \left( (4)^{3/2} - (3)^{3/2} \right) = \frac{2}{3} (8 - 3\sqrt{3})\)
For\(\int_0^1 \sqrt{1 + x} \, dx\):
\(\int \sqrt{1 + x} \, dx = \frac{2}{3} (1 + x)^{3/2}\)
Evaluating from 0 to 1:
\(\frac{2}{3} \left( (1 + x)^{3/2} \right) \Big|_0^1 = \frac{2}{3} \left( (2)^{3/2} - (1)^{3/2} \right) = \frac{2}{3} (2\sqrt{2} - 1)\)
Step 4. Combining the Results:
\(\frac{1}{2} \left( \frac{2}{3} (8 - 3\sqrt{3}) - \frac{2}{3} (2\sqrt{2} - 1) \right)\)
Simplifying:
\(\frac{1}{3} (8 - 3\sqrt{3} - 2\sqrt{2} + 1) = \frac{1}{3} (9 - 3\sqrt{3} - 2\sqrt{2})\)
Thus:
\(a = 3, \quad b = -\frac{2}{3}, \quad c = -1\)
Step 5. Calculating \( 2a + 3b - 4c \):
\(2a + 3b - 4c = 2 \times 3 + 3 \times \left( -\frac{2}{3} \right) - 4 \times (-1)\)
\(= 6 − 2 + 4 = 8\)
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,